Research paper
TheoreticalComputed Band StructureQuantum valley Hall states in low-buckled counterparts of graphene bilayer
Yu-Hao Shen, Jun-Ding Zheng, Wen-Yi Tong, Zhi-Qiang Bao et al.
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Each sample groups how it was prepared, characterized, and measured. Click a card to expand.
1 characterization4 properties1 figure
1 property
| Type | Label | Value | Material | Sample | Condition | Source |
|---|---|---|---|---|---|---|
| Valley Chern Number | Cv | 0 | — | |||
| Valley Chern Number | Cv | 2 | — | |||
| Topological Invariant Z2 | Z₂ | 0 | — | |||
| Phase Transition Boundary Parameter | analytic transition boundary | (m0,m1) boundary given by 4(m0-m1)^2 = λ''_SOC^2 + 4(λ_SOC)^2 | — | |||
| Band Inversion | K-band inversion in mini BZ | true | — |
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Effects of phonon confinement on electron transport in Si nanowire and armchair-edge graphene nanoribbon transistors: A dissipative quantum-transport study
Topological phase diagram of the Haldane model on a Bishamon-kikko–honeycomb lattice
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SOLAR CELL WITH GRAPHENE-SILICON QUANTUM DOT HYBRID STRUCTURE AND METHOD OF MANUFACTURING THE SAME
Each sample groups how it was prepared, characterized, and measured. Click a card to expand.
1 characterization4 properties1 figure
1 property
| Type | Label | Value | Material | Sample | Condition | Source |
|---|---|---|---|---|---|---|
| Valley Chern Number | Cv | 0 | — | |||
| Valley Chern Number | Cv | 2 | — | |||
| Topological Invariant Z2 | Z₂ | 0 | — | |||
| Phase Transition Boundary Parameter | analytic transition boundary | (m0,m1) boundary given by 4(m0-m1)^2 = λ''_SOC^2 + 4(λ_SOC)^2 | — | |||
| Band Inversion | K-band inversion in mini BZ | true | — |
Related documents with shared materials, methods, properties, or citations.
Light-engineered Multichannel Quantum Anomalous Hall Effect in High-order Topological Plumbene
Quantum Computation of the Electronic Structure of Some Prototype Solids
Effects of self-consistent extended Hubbard interactions and spin-orbit couplings on energy bands of semiconductors and topological insulators
Orbital-Selective Engineering of Strain-Tunable Chern Insulators in Momentum Space
Wide-mode-area slow light waveguides in valley photonic crystal heterostructures
Electric field tunable magnetoexcitons in Xenes/hBN/TMDC, Xenes/hBN/BP, and Xenes/hBN/TMTC heterostructures
Effects of phonon confinement on electron transport in Si nanowire and armchair-edge graphene nanoribbon transistors: A dissipative quantum-transport study
Topological phase diagram of the Haldane model on a Bishamon-kikko–honeycomb lattice
Band-selective simulation of photoelectron intensity and converging Berry phase in trilayer graphene
SOLAR CELL WITH GRAPHENE-SILICON QUANTUM DOT HYBRID STRUCTURE AND METHOD OF MANUFACTURING THE SAME
Each sample groups how it was prepared, characterized, and measured. Click a card to expand.
1 characterization4 properties1 figure
1 property
| Type | Label | Value | Material | Sample | Condition | Source |
|---|---|---|---|---|---|---|
| Valley Chern Number | Cv | 0 | — | |||
| Valley Chern Number | Cv | 2 | — | |||
| Topological Invariant Z2 | Z₂ | 0 | — | |||
| Phase Transition Boundary Parameter | analytic transition boundary | (m0,m1) boundary given by 4(m0-m1)^2 = λ''_SOC^2 + 4(λ_SOC)^2 | — | |||
| Band Inversion | K-band inversion in mini BZ | true | — |
Related documents with shared materials, methods, properties, or citations.
Light-engineered Multichannel Quantum Anomalous Hall Effect in High-order Topological Plumbene
Quantum Computation of the Electronic Structure of Some Prototype Solids
Effects of self-consistent extended Hubbard interactions and spin-orbit couplings on energy bands of semiconductors and topological insulators
Orbital-Selective Engineering of Strain-Tunable Chern Insulators in Momentum Space
Wide-mode-area slow light waveguides in valley photonic crystal heterostructures
Electric field tunable magnetoexcitons in Xenes/hBN/TMDC, Xenes/hBN/BP, and Xenes/hBN/TMTC heterostructures
Effects of phonon confinement on electron transport in Si nanowire and armchair-edge graphene nanoribbon transistors: A dissipative quantum-transport study
Topological phase diagram of the Haldane model on a Bishamon-kikko–honeycomb lattice
Band-selective simulation of photoelectron intensity and converging Berry phase in trilayer graphene
SOLAR CELL WITH GRAPHENE-SILICON QUANTUM DOT HYBRID STRUCTURE AND METHOD OF MANUFACTURING THE SAME
Each sample groups how it was prepared, characterized, and measured. Click a card to expand.
1 characterization4 properties1 figure
1 property
| Type | Label | Value | Material | Sample | Condition | Source |
|---|---|---|---|---|---|---|
| Valley Chern Number | Cv | 0 | — | |||
| Valley Chern Number | Cv | 2 | — | |||
| Topological Invariant Z2 | Z₂ | 0 | — | |||
| Phase Transition Boundary Parameter | analytic transition boundary | (m0,m1) boundary given by 4(m0-m1)^2 = λ''_SOC^2 + 4(λ_SOC)^2 | — | |||
| Band Inversion | K-band inversion in mini BZ | true | — |
Related documents with shared materials, methods, properties, or citations.
Light-engineered Multichannel Quantum Anomalous Hall Effect in High-order Topological Plumbene
Quantum Computation of the Electronic Structure of Some Prototype Solids
Effects of self-consistent extended Hubbard interactions and spin-orbit couplings on energy bands of semiconductors and topological insulators
Orbital-Selective Engineering of Strain-Tunable Chern Insulators in Momentum Space
Wide-mode-area slow light waveguides in valley photonic crystal heterostructures
Electric field tunable magnetoexcitons in Xenes/hBN/TMDC, Xenes/hBN/BP, and Xenes/hBN/TMTC heterostructures
Effects of phonon confinement on electron transport in Si nanowire and armchair-edge graphene nanoribbon transistors: A dissipative quantum-transport study
Topological phase diagram of the Haldane model on a Bishamon-kikko–honeycomb lattice
Band-selective simulation of photoelectron intensity and converging Berry phase in trilayer graphene
SOLAR CELL WITH GRAPHENE-SILICON QUANTUM DOT HYBRID STRUCTURE AND METHOD OF MANUFACTURING THE SAME